{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:FME6WM7DSUJRZHA2BUVBEVQIZW","short_pith_number":"pith:FME6WM7D","schema_version":"1.0","canonical_sha256":"2b09eb33e395131c9c1a0d2a125608cd82bd3de2d0a84e7f1e82b938e097aefd","source":{"kind":"arxiv","id":"hep-ph/9610266","version":1},"attestation_state":"computed","paper":{"title":"Heavy-Quark Effective Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matthias Neubert (CERN)","submitted_at":"1996-10-07T13:23:00Z","abstract_excerpt":"We give an introduction to the heavy-quark effective theory and the $1/m_Q$ expansion, which provide the modern framework for a systematic, model-independent description of the properties and decays of hadrons containing a heavy quark. We discuss the applications of these concepts to spectroscopy and to the weak decays of $B$ mesons."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9610266","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-07T13:23:00Z","cross_cats_sorted":[],"title_canon_sha256":"5bab5d0662bfa4d54e5f9034b3ed67666a922371111f4e1678a00a8d614a2588","abstract_canon_sha256":"e17629842ccc750b39e884e319913fb45bfaa48cb73ef565998c0a3ac964f30f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:30:04.188088Z","signature_b64":"rIFMK+Kf2OquM79R6ejiN4ug+C1n2DfWCELjRnjc5WHWlYWRbAqZZDS7Wz5VGKZOLnQ5ScPZj9gjLoN7U0LRCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2b09eb33e395131c9c1a0d2a125608cd82bd3de2d0a84e7f1e82b938e097aefd","last_reissued_at":"2026-07-04T14:30:04.187661Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:30:04.187661Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy-Quark Effective Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matthias Neubert (CERN)","submitted_at":"1996-10-07T13:23:00Z","abstract_excerpt":"We give an introduction to the heavy-quark effective theory and the $1/m_Q$ expansion, which provide the modern framework for a systematic, model-independent description of the properties and decays of hadrons containing a heavy quark. We discuss the applications of these concepts to spectroscopy and to the weak decays of $B$ mesons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9610266","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9610266/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9610266","created_at":"2026-07-04T14:30:04.187719+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9610266v1","created_at":"2026-07-04T14:30:04.187719+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9610266","created_at":"2026-07-04T14:30:04.187719+00:00"},{"alias_kind":"pith_short_12","alias_value":"FME6WM7DSUJR","created_at":"2026-07-04T14:30:04.187719+00:00"},{"alias_kind":"pith_short_16","alias_value":"FME6WM7DSUJRZHA2","created_at":"2026-07-04T14:30:04.187719+00:00"},{"alias_kind":"pith_short_8","alias_value":"FME6WM7D","created_at":"2026-07-04T14:30:04.187719+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2606.30737","citing_title":"$\\Lambda \\bar \\Lambda$ spin correlations in high-energy collisions from quantum channels: an open quantum system view of hadronization","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"2606.28702","citing_title":"Heavy mesons from the QCD instanton vacuum beyond the static limit","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2006.00200","citing_title":"Analysis of the QCD Kondo phase using random matrices","ref_index":35,"is_internal_anchor":true},{"citing_arxiv_id":"2604.12603","citing_title":"Open-flavor threshold effects on quarkonium spectrum in the BOEFT","ref_index":142,"is_internal_anchor":true},{"citing_arxiv_id":"2604.06088","citing_title":"Comments on Symmetry Operators, Asymptotic Charges and Soft Theorems","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW","json":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW.json","graph_json":"https://pith.science/api/pith-number/FME6WM7DSUJRZHA2BUVBEVQIZW/graph.json","events_json":"https://pith.science/api/pith-number/FME6WM7DSUJRZHA2BUVBEVQIZW/events.json","paper":"https://pith.science/paper/FME6WM7D"},"agent_actions":{"view_html":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW","download_json":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW.json","view_paper":"https://pith.science/paper/FME6WM7D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9610266&json=true","fetch_graph":"https://pith.science/api/pith-number/FME6WM7DSUJRZHA2BUVBEVQIZW/graph.json","fetch_events":"https://pith.science/api/pith-number/FME6WM7DSUJRZHA2BUVBEVQIZW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW/action/storage_attestation","attest_author":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW/action/author_attestation","sign_citation":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW/action/citation_signature","submit_replication":"https://pith.science/pith/FME6WM7DSUJRZHA2BUVBEVQIZW/action/replication_record"}},"created_at":"2026-07-04T14:30:04.187719+00:00","updated_at":"2026-07-04T14:30:04.187719+00:00"}